Schur polynomials of infinitely many time-variables are among the most important special functions of modern mathematical physics. They are directly associated with the characters of linear and symmetric group and are therefore labeled by Young diagrams. They possess a somewhat mysterious deformation to Macdonald and Kerov polynomials, which no longer has grouptheory interpretation, still preserves most of the nice properties of Schur functions. The family of Schur-Macdonald function, however, is not big enough -needed for various applications are counterparts of the Schur functions, labeled by plane (3d) partitions. Recently a very concrete suggestion was made on how this generalization can be done -and miraculous coincidences on this way can serve as a support to the idea, which, however, needs a lot of work to become a reliable and efficient theory. In particular, one can expect that Macdonald and even entire Kerov deformations should appear in this theory on equal right with the ordinary 2-Schur functions. In this paper we demonstrate in some detail how this works for Macdonald polynomials and how they emerge from the 3-Schur functions when the vector time-variables, associated with plane-partitions, are projected onto the ordinary scalar times under non-vanishing angles, which depend on q and t. We also explain how the cut-and-join operators smoothly interpolate between different cases. Most of consideration is restricted to level two. +